Book Chapter10.1016/S0081-1947(08)60529-9
X-Ray Diffraction Studies of the Lattice Parameters of Solids under Very High Pressure
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TL;DR: In this article, the measurements of lattice parameters versus pressure made in this laboratory were discussed, primarily, the measurements were made by measuring the lattice parameter of a "marker" along with those of the substance studied.
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Abstract: Publisher Summary This chapter discusses, primarily, the measurements of lattice parameters versus pressure made in this laboratory. The apparatus used permits a rather large range of pressure. (When studying a single cubic metal of low compressibility such as Ag, Nb, or Mo where one or two lines suffice, pressures of 550 kbar or more have, on occasion, been obtained. For substances where more lines are necessary, or for mixtures of substances, the range is more limited.) Some of the other methods of measurement permit more accuracy in the low-pressure region. There are no primary pressure standards in the very high pressure range. Pressures are established in this work by measuring the lattice parameter of a “marker” along with those of the substance studied. Commonly used markers include cubic metals such as Al, Ag, Nb, Mo, and Pd, where shock-wave densities corrected to room temperature have been shown to be internally consistent. Salts such as NaCl, MgO, NaF, and LiF that have been studied using these metallic markers have been utilized themselves to measure pressure. Markers are selected which have “windows” (spaces with no lines) in regions where the sample have prominent lines. Also, more compressible markers are used to establish more accurate pressures in the low-pressure region.
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Citations
Finite strain isotherm and velocities for single-crystal and polycrystalline NaCl at high pressures and 300°K
TL;DR: In this article, a large portion of the data is consistent, to within reasonable uncertainties, with the Eulerian formulation of finite strain, in the BE2 form, which contains three parameters, of which two, K0 and K0′, are obtainable from single-crystal ultrasonic measurements, while the third, K 0″, may be found with the aid of shock wave data.
2.6K
Graphite under pressure: Equation of state and first-order Raman modes.
TL;DR: Using the a- and c-axis compression data, the dependence of phonon frequencies on intralayer and interlayer separation is determined and a stronger anharmonicity of this mode is indicated.
572
Pressure-Induced Phonon Frequency Shifts Measured by Raman Scattering
TL;DR: In this article, pressure shifts of longwavelength LO and TO phonons of a number of diamond-, zinc-blende-, and wurtzite-type crystals as functions of hydrostatic pressure have been investigated by Raman-scattering measurements.
263
References
Energy of Cohesion, Compressibility, and the Potential Energy Functions of the Graphite System
L. A. Girifalco,R. A. Lad +1 more
TL;DR: In this paper, the potential energy of graphite lattice summations of importance in the graphite system have been computed by direct summation assuming a Lennard-Jones 6-12 potential between carbon atoms.
618
Equation of State for Nineteen Metallic Elements from Shock‐Wave Measurements to Two Megabars
R. G. McQueen,S. P. Marsh +1 more
TL;DR: In this paper, the authors extended the Hugoniot loci into the one-to-two-megabar region for 19 metallic elements: Ag, Au, Cd, Co, Cr, Cu, Mo, Ni, Pb, Sn, Th, Ti, Tl, V, W, Zn, Bi, Fe, Sb.
607
Direct Transformation of Hexagonal Boron Nitride to Denser Forms
F. P. Bundy,R. H. Wentorf +1 more
TL;DR: In this paper, a hexagonal, graphitelike boron nitride was changed directly into the zincblende cubic form reported earlier or into a new wurtzite form by the application of static high pressures.
522
Elastic Moduli of Quartz versus Hydrostatic Pressure at 25° and − 195.8°C
TL;DR: In this article, a set of adjusted velocities and initial pressure derivatives was obtained which satisfies all the cross-checks exactly, while minimizing a weighted sum of the squares of the adjustments from the measured values.
480